{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:ZBWVMUK3OMU7TB4PDQR72EVF2B","short_pith_number":"pith:ZBWVMUK3","canonical_record":{"source":{"id":"1611.08670","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-11-26T06:50:20Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"22e881635063c3b86bbea2c607e16f584867fbd18c6314b5bf0d44f5fceeb060","abstract_canon_sha256":"58cdc7a1604338b3a83253df33e2fb634ba471e5c544ac1bab86f67c73d5c96b"},"schema_version":"1.0"},"canonical_sha256":"c86d56515b7329f9878f1c23fd12a5d0717fab950037cefc42a076e12b5ded16","source":{"kind":"arxiv","id":"1611.08670","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1611.08670","created_at":"2026-05-18T00:54:04Z"},{"alias_kind":"arxiv_version","alias_value":"1611.08670v3","created_at":"2026-05-18T00:54:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.08670","created_at":"2026-05-18T00:54:04Z"},{"alias_kind":"pith_short_12","alias_value":"ZBWVMUK3OMU7","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_16","alias_value":"ZBWVMUK3OMU7TB4P","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_8","alias_value":"ZBWVMUK3","created_at":"2026-05-18T12:30:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:ZBWVMUK3OMU7TB4PDQR72EVF2B","target":"record","payload":{"canonical_record":{"source":{"id":"1611.08670","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-11-26T06:50:20Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"22e881635063c3b86bbea2c607e16f584867fbd18c6314b5bf0d44f5fceeb060","abstract_canon_sha256":"58cdc7a1604338b3a83253df33e2fb634ba471e5c544ac1bab86f67c73d5c96b"},"schema_version":"1.0"},"canonical_sha256":"c86d56515b7329f9878f1c23fd12a5d0717fab950037cefc42a076e12b5ded16","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:54:04.571219Z","signature_b64":"/leL0so8nHkKdqcpeDz/2RT3Y9fmd7DIWs+d7nlE42QONFzuFTeU1YAw6s8IA74R7s7VIhF1cH07VzeEFsuqDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c86d56515b7329f9878f1c23fd12a5d0717fab950037cefc42a076e12b5ded16","last_reissued_at":"2026-05-18T00:54:04.570605Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:54:04.570605Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1611.08670","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:54:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qzZprT6JUFLp/YkV6LbBFgQ/+fv8LEGmlLTkdlHJTSqeDzVBdhHcreHHrYl75R5OQkdb3wR4jXU173iKbqz1Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-20T07:41:20.676294Z"},"content_sha256":"d520ee1768db9bed84bf2225f85f8d1d70ea1ee278920467772134bb2b26a4ce","schema_version":"1.0","event_id":"sha256:d520ee1768db9bed84bf2225f85f8d1d70ea1ee278920467772134bb2b26a4ce"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:ZBWVMUK3OMU7TB4PDQR72EVF2B","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Landau damping of surface plasmons in metal nanostructures","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"cond-mat.mes-hall","authors_text":"Tigran V. Shahbazyan","submitted_at":"2016-11-26T06:50:20Z","abstract_excerpt":"We develop a quantum-mechanical theory for Landau damping of surface plasmons in metal nanostructures larger that the characteristic length for nonlocal effects. We show that the electron surface scattering, which facilitates plasmon decay in small nanostructures, can be incorporated into the metal dielectric function on par with phonon and impurity scattering. The derived surface scattering rate is determined by the plasmon local field polarization relative to the metal-dielectric interface and is highly sensitive to the system geometry. We illustrate our model by providing analytical results"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.08670","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:54:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ik/MiHo69D1HDg5jUddN17+oOZOOB4S2/6ZkKj69XFoNgf8jVv/nOTEraQunz9qsTBpPaj8HyiRpwzgPinWpCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-20T07:41:20.676663Z"},"content_sha256":"20771a3471c4aad8c7dfe45ccf2dfd29850d1942a914d79165c0d57e5f751199","schema_version":"1.0","event_id":"sha256:20771a3471c4aad8c7dfe45ccf2dfd29850d1942a914d79165c0d57e5f751199"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZBWVMUK3OMU7TB4PDQR72EVF2B/bundle.json","state_url":"https://pith.science/pith/ZBWVMUK3OMU7TB4PDQR72EVF2B/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZBWVMUK3OMU7TB4PDQR72EVF2B/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-20T07:41:20Z","links":{"resolver":"https://pith.science/pith/ZBWVMUK3OMU7TB4PDQR72EVF2B","bundle":"https://pith.science/pith/ZBWVMUK3OMU7TB4PDQR72EVF2B/bundle.json","state":"https://pith.science/pith/ZBWVMUK3OMU7TB4PDQR72EVF2B/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZBWVMUK3OMU7TB4PDQR72EVF2B/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:ZBWVMUK3OMU7TB4PDQR72EVF2B","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"58cdc7a1604338b3a83253df33e2fb634ba471e5c544ac1bab86f67c73d5c96b","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-11-26T06:50:20Z","title_canon_sha256":"22e881635063c3b86bbea2c607e16f584867fbd18c6314b5bf0d44f5fceeb060"},"schema_version":"1.0","source":{"id":"1611.08670","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1611.08670","created_at":"2026-05-18T00:54:04Z"},{"alias_kind":"arxiv_version","alias_value":"1611.08670v3","created_at":"2026-05-18T00:54:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.08670","created_at":"2026-05-18T00:54:04Z"},{"alias_kind":"pith_short_12","alias_value":"ZBWVMUK3OMU7","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_16","alias_value":"ZBWVMUK3OMU7TB4P","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_8","alias_value":"ZBWVMUK3","created_at":"2026-05-18T12:30:53Z"}],"graph_snapshots":[{"event_id":"sha256:20771a3471c4aad8c7dfe45ccf2dfd29850d1942a914d79165c0d57e5f751199","target":"graph","created_at":"2026-05-18T00:54:04Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We develop a quantum-mechanical theory for Landau damping of surface plasmons in metal nanostructures larger that the characteristic length for nonlocal effects. We show that the electron surface scattering, which facilitates plasmon decay in small nanostructures, can be incorporated into the metal dielectric function on par with phonon and impurity scattering. The derived surface scattering rate is determined by the plasmon local field polarization relative to the metal-dielectric interface and is highly sensitive to the system geometry. We illustrate our model by providing analytical results","authors_text":"Tigran V. Shahbazyan","cross_cats":["physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-11-26T06:50:20Z","title":"Landau damping of surface plasmons in metal nanostructures"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.08670","kind":"arxiv","version":3},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:d520ee1768db9bed84bf2225f85f8d1d70ea1ee278920467772134bb2b26a4ce","target":"record","created_at":"2026-05-18T00:54:04Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"58cdc7a1604338b3a83253df33e2fb634ba471e5c544ac1bab86f67c73d5c96b","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-11-26T06:50:20Z","title_canon_sha256":"22e881635063c3b86bbea2c607e16f584867fbd18c6314b5bf0d44f5fceeb060"},"schema_version":"1.0","source":{"id":"1611.08670","kind":"arxiv","version":3}},"canonical_sha256":"c86d56515b7329f9878f1c23fd12a5d0717fab950037cefc42a076e12b5ded16","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c86d56515b7329f9878f1c23fd12a5d0717fab950037cefc42a076e12b5ded16","first_computed_at":"2026-05-18T00:54:04.570605Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:54:04.570605Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"/leL0so8nHkKdqcpeDz/2RT3Y9fmd7DIWs+d7nlE42QONFzuFTeU1YAw6s8IA74R7s7VIhF1cH07VzeEFsuqDw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:54:04.571219Z","signed_message":"canonical_sha256_bytes"},"source_id":"1611.08670","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d520ee1768db9bed84bf2225f85f8d1d70ea1ee278920467772134bb2b26a4ce","sha256:20771a3471c4aad8c7dfe45ccf2dfd29850d1942a914d79165c0d57e5f751199"],"state_sha256":"20f72ef147cc1648a0318948428b3fdf713076c8ba2fd8c88c3396b22972f3b8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AzYgPY6Mw42g7Z7qHHLE1M5WpG48Gw+ZzXHzsY/GCaJuUYqeNyiJwzuAfgE5u7pYvn64bq0bLcvx+3z/XUgVCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-20T07:41:20.678618Z","bundle_sha256":"00a3abebf8d567595e5529343c6863049ef4ea0555c81c0a7722846c630650f4"}}